PHY138 – Waves, Lecture 8 Today’s overview: Dispersion and Rainbows Lenses The Thin Lens Equation Lenses used in Combination

Course Evaluations in Tutorial this week! Your chance to officially evaluate Vatche and me is this week during tutorial. Your comments will make it into the 2008-09 Anti-Calendar and will form part of the tenure-review for me and Vatche. You participation and honest comments are appreciated – we will read them in the summer after the marks have been submitted.

Dispersion

Light going through a prism bends toward the base 2 1 1 n =1 Bending angle depends on value of n 1 2

Rainbows

Lenses Formed by two curved boundaries between transparent media. Lenses often have spherical surfaces (lens-maker’s equation). The curved surfaces are parts of large spheres of radius R1 or R2. Every lens shaped like a circle has a diameter, D, and focal length, f. The ratio of (f / D) is called “f-number”. For example, an “f/6” lens has a focal length of 6 times its diameter.

Converging Lens Focal length, f Focal Point NOTE: Focal length is defined for initially parallel rays.

Diverging Lens Negative Focal length, -f Virtual Focal Point Rays appear to emerge from Virtual Focal Point

Diverging rays through a Converging Lens Focal length, f This follows from the principle of reversibility.

They will remain parallel. They will diverge (spread out). f What will happen to the rays emerging to the right of the lens if the face is moved a little closer to the lens? They will remain parallel. They will diverge (spread out). They will converge (toward a focus).

They will remain parallel. They will diverge (spread out). f What will happen to the rays emerging to the right of the lens if the face is moved a little further away from the lens? They will remain parallel. They will diverge (spread out). They will converge (toward a focus).

Diverging rays through a Converging Lens Focal length, f s s’ Thin Lens Equation:

Thin Lens Equation: sign conventions image object f s s’ s is positive for objects to the left of lens, negative for objects to the right of lens (virtual objects). s’ is positive for images to the right of lens, negative for images to the left of lens (virtual images). f is positive for converging lenses, negative for diverging lenses.

Lenses used in combination If one or more lenses are used in combination, the object of the second lens is the image of the first lens. The thin lens equation can be applied to several lenses in sequence, always setting the image of the previous lens to be the object of the next.